QUANTUM
ORCHESTRATION PLATFORM

The Quantum Orchestration Platform is a whole new paradigm for quantum control and is fundamentally different from general-purpose test equipment like AWGs, lock-ins, digitizers, etc. The main differences are:

1. The span of quantum experiments & algorithms which can be run out-of-the-box
2. The pace of the research and development
3. The level of adequacy of the specific specs & capabilities required for quantum research & development (e.g like latency, run-time, etc)

1) The span of quantum experiments & algorithms which can be run out-of-the-box

We like to think of the span of experiments & algorithms which a system can run as the subspace of the experimental phase-space that it covers. While AWGs, Lock-ins, digitizers cover specific points or small regions in this phase space, the quantum orchestration platform covers it entirely. In other words, each general-purpose test tool, even if it is re-branded as a quantum controller, has a fixed set of allowable functions. The Quantum Orchestration Platform (QOP)  however, is a full-stack system allowing you to easily and quickly run even your dream experiments and real-time sequences out-of-the-box, from a high-level programming language, QUA. In most cases, each test and measure tool can be expressed and implemented as a single QUA program that can run on the QOP. Alternatively, each such instrument can be described by omitting a different subspace of the full QOP’s phase-space.

2) The pace of the research and development

Every once in a while you have a new brilliant idea for an experiment. While these ideas are more groundbreaking, they are also more challenging and end up being outside the scope of your general-purpose test equipment (its subspace). Once this happens, you have 3 choices:

1. Repurpose your general-purpose. It appears that in all labs such repurposing draws an incredible amount of time and resources, which comes at the expense of the physics and science to be explored. Whether it’s FPGA programming, coding libraries, dealing with drivers, or synchronizing different modules, labs spend years of work on repurposing general-purpose AWGs, Lock-ins, and digitizers for quantum control. It’s often required even for the simplest Ramsey and spectroscopy, and it’s always a must when it comes to multi-axes tomography, the 2-qubit RB sequence, and all the way to multi-qubit quantum-error-correction. We’ve met students who themselves spent months and years doing so. We actually did it ourselves!
2. Give up your brilliant idea and introduce a new constraint for your ideas’ phase-space. It must comply with the experimental phase-space covered by your existing control system.
3. Get an OPX! We firmly believe that scientific progress relies on ideas, but also on the capabilities of the tools we use. Even our ideas in many cases stem from what we define as technically possible. Our goal at QM is to let you imagine any experiment, the most groundbreaking research, and the most sought-for flagship papers, and always know: yes, of course, it can run. Right out of the box!

In experimental physics, there are many bottlenecks. Long fabrication processes, mirrors alignment (and re-alignment!), helium leakages, vacuum-chamber baking, lead times of crucial equipment, and last but not least: in-house development of quantum control capabilities. Specifically, in quantum computing, the control layer can either be an enabler to progress rapidly and run even the most complex experiments seamlessly or be one of the leading bottlenecks in the lab. Our mission is to allow all teams to run even the wildest experiments of their dreams seamlessly and push the boundaries of the physics they can explore to a whole new level. 

3) The level of adequacy for the specific specs & capabilities required for quantum research & development

The general-purpose equipment available today was not built for quantum. In the best-case scenario, it was rebranded. AWGs, lock-ins, and digitizers are used for communication systems, lidars, medical device research, and the list goes on. Of course, we don’t mind non-quantum-experimentalists using the same machines, but this has several consequences. First,  these machines are limited in the feature-set they provide. They are also misaligned with the requirements of quantum computing by not supplying you with the critical features you require. And finally, they equip you with quite a few features you simply don’t need (that you’re still paying for). The QOP full-stack quantum control hardware and software and all of its features was created by quantum physicists for quantum physicists, with your experimental needs in mind. 

The Quantum Orchestration Platform is a whole new paradigm for quantum control and is fundamentally different from general-purpose test equipment like AWGs, lock-ins, digitizers, etc. The main differences are:

1. The span of quantum experiments & algorithms which can be run out-of-the-box
2. The pace of the research and development
3. The level of adequacy of the specific specs & capabilities required for quantum research & development (e.g like latency, run-time, etc)

1) The span of quantum experiments & algorithms which can be run out-of-the-box

We like to think of the span of experiments & algorithms which a system can run as the subspace of the experimental phase-space that it covers. While AWGs, Lock-ins, digitizers cover specific points or small regions in this phase space, the quantum orchestration platform covers it entirely. In other words, each general-purpose test tool, even if it is re-branded as a quantum controller, has a fixed set of allowable functions. The Quantum Orchestration Platform (QOP)  however, is a full-stack system allowing you to easily and quickly run even your dream experiments and real-time sequences out-of-the-box, from a high-level programming language, QUA. In most cases, each test and measure tool can be expressed and implemented as a single QUA program that can run on the QOP. Alternatively, each such instrument can be described by omitting a different subspace of the full QOP’s phase-space.

2) The pace of the research and development

Every once in a while you have a new brilliant idea for an experiment. While these ideas are more groundbreaking, they are also more challenging and end up being outside the scope of your general-purpose test equipment (its subspace). Once this happens, you have 3 choices:

1. Repurpose your general-purpose. It appears that in all labs such repurposing draws an incredible amount of time and resources, which comes at the expense of the physics and science to be explored. Whether it’s FPGA programming, coding libraries, dealing with drivers, or synchronizing different modules, labs spend years of work on repurposing general-purpose AWGs, Lock-ins, and digitizers for quantum control. It’s often required even for the simplest Ramsey and spectroscopy, and it’s always a must when it comes to multi-axes tomography, the 2-qubit RB sequence, and all the way to multi-qubit quantum-error-correction. We’ve met students who themselves spent months and years doing so. We actually did it ourselves!
2. Give up your brilliant idea and introduce a new constraint for your ideas’ phase-space. It must comply with the experimental phase-space covered by your existing control system.
3. Get an OPX! We firmly believe that scientific progress relies on ideas, but also on the capabilities of the tools we use. Even our ideas in many cases stem from what we define as technically possible. Our goal at QM is to let you imagine any experiment, the most groundbreaking research, and the most sought-for flagship papers, and always know: yes, of course, it can run. Right out of the box!

In experimental physics, there are many bottlenecks. Long fabrication processes, mirrors alignment (and re-alignment!), helium leakages, vacuum-chamber baking, lead times of crucial equipment, and last but not least: in-house development of quantum control capabilities. Specifically, in quantum computing, the control layer can either be an enabler to progress rapidly and run even the most complex experiments seamlessly or be one of the leading bottlenecks in the lab. Our mission is to allow all teams to run even the wildest experiments of their dreams seamlessly and push the boundaries of the physics they can explore to a whole new level. 

3) The level of adequacy for the specific specs & capabilities required for quantum research & development

The general-purpose equipment available today was not built for quantum. In the best-case scenario, it was rebranded. AWGs, lock-ins, and digitizers are used for communication systems, lidars, medical device research, and the list goes on. Of course, we don’t mind non-quantum-experimentalists using the same machines, but this has several consequences. First,  these machines are limited in the feature-set they provide. They are also misaligned with the requirements of quantum computing by not supplying you with the critical features you require. And finally, they equip you with quite a few features you simply don’t need (that you’re still paying for). The QOP full-stack quantum control hardware and software and all of its features was created by quantum physicists for quantum physicists, with your experimental needs in mind. 

Multiple pulsers can be combined and sent to the same output port, thereby generating a fully, real-time controllable multi-tone pulse capable of, for instance, driving an Acousto Optic Deflector (AOD) in order to perform parallel atom arrangements on a tweezer array. 

The flexible QUA programming language allows you to easily implement any atom-sorting algorithm you can think of (using less than ~100 lines of code and without the need to configure DDSs or write FPGA code to drive SDRs).

Of course! Such systems can co-exist with the Quantum Orchestration Platform in three different ways:

1. Suppose you wish to synchronize other instruments with the OPX for them to work on the same clock and work simultaneously (e.g play pulses to different qubits simultaneously from the OPX and an AWG). In that case, you can use one or several digital output ports of the OPX as triggers. For example, you can run a very complex pulse sequence including playing pulses, doing Bayesian estimations, time tagging, etc., and simply trigger another AWG to play some of the needed pulses in the course of the sequence.
   
2. Suppose you want to run a multi-axes protocol in which, for instance, the outer loop is an external device (e.g Yokogawa, or another low-frequency source) and the inner-loop is a QUA program. In that case, you can do it synchronously by using the QUA commands pause() and resume(). This is very easy to do.
   
3. One last and very convenient feature for synchronizing with other instruments is employing the digital inputs of the OPX. Then, you can trigger the OPX from an external device and use the QUA command wait_for_trigger() so that you can hold any program at any point and wait for an external signal to arrive.

The pulse-processor orchestrates all the waveform generation, waveform acquisition, classical processing, and control flow in real-time. But what is its API? 

The API for the pulse processor is QUA: a powerful yet intuitive quantum programming language. In QUA you can formulate any protocol/experiment – from spectroscopy to quantum-error-correction. Once the program is formulated it is compiled by the XQP compiler to the assembly language of the pulse processor. Next, the program, now formulated in the pulse processor’s assembly language, is sent to the pulse processor which runs it in real-time.

Using the intuitive QUA language and our compiler, you can now directly and intuitively code complex sequences from a high-level programming language, including real-time feedback, classical calculations (Turing-complete), comprehensive control flow, etc. 

As physicists, we always like to ask the more fundamental questions, even when at first glance they seem trivial. In order to answer “what is the pulse processor,” it is useful to first answer the trivial question “what is a quantum experiment?”This is because the pulse processor was architected from the ground-up to run even the most complex quantum experiments one could think of. Now, let’s break-down a quantum experiment to four main components:

1. Gates – The different terms in the Hamiltonian which cause the sought time-evolution. These gates are usually performed by directing well-crafted pulses (laser, microwave) to the qubits.
2. Measurements – Since you’re a classical being, at some point, you will have to collapse the system so you can “see it for yourself”. The measurements are performed in various ways – ADCs, SPCMs, PDs, cameras, etc.
3. Classical processing – There is no quantum processing without classical processing. Whether it’s demodulation, integration, time-tagging, TTL, counting, state estimations, error-estimations, Bayesian estimations, or even arithmetics as simple as \tau=\tau+5 when looping over the time difference in a Ramsey sequence. There is not a single quantum protocol that does not require classical processing.
4. Control flow – the good-old if/else, while, for, cases, etc. From the simplest averaging loop and parameter-sweep loop, through active-reset and to multi-qubit error correction employing a multitude of nested if/else’s. Control-flow is indispensable for quantum protocols.
   

Every quantum experiment (or protocol) is a combination of these four elements. Every quantum protocol is an entangled sequence of gates, measurements, and classical processing, all combined in various ways and wrapped with various control-flow statements. And someone has to orchestrate all that!

The Pulse Processor is a processor architected to run sequences that combine all the above in real-time, in a perfectly synchronized and orchestrated way. That includes:

1. Waveform generation in a fully parametric manner. Namely, the pulse processor does not need you to load all the pulses in advance, but rather it generates them in real-time as defined by the program. In other words, the pulse processor directly processes pulses as opposed to simply shoving them into memory.
2. Waveform acquisition including the acquisition of both analog data (through ADCs) and digital data (from SPCMs, PDs, camera, etc). Including continuous acquisition for CW measurements or qubit-tracking (and weak measurements) as well as pulsed acquisition in synchronization with the waveform generation and real-time processing. 
3. Real-time processing including real-time processing of acquired data (e.g weighted demodulators and integrations, image-processing, TTL counting, time-tagging, etc), state-estimations, and even neural networks.
4. Control flow including everything you typically do in MATLAB/python, now running in real-time, at time scales that are faster than your qubits (10s of nanoseconds)! Nested loops, complex branching trees with countless if/else’s, to form the most complex protocol you may have in mind.

And above all, these four elements are NOT to be regarded as independent. Quantum protocols are an interacting system, where waveform generation leads to waveform acquisition, followed by classical processing which then affects the following generated pulses. And many such threads running in parallel, and affecting each other as well.

To enable such performance, the pulse processor is built in a multi-core architecture containing several pulsers. Each pulser is an independent real-time core capable of driving one or more quantum elements (qubits, collective modes, two-/multi-level transitions, resonators, etc.). Every pulser is essentially a specialized processing unit that may simultaneously handle both waveform generation, waveform acquisition, and all the real-time calculations (classical processing) required (it is Turing complete!) in a deterministic manner and with ultra-low latency.

The Quantum Orchestration Platform (QOP) is a modular architecture, allowing you to add several OPX machines to scale up based on your quantum control needs. A single unit is composed of up to 10 digital outputs, 10 analog outputs, and 2 analog inputs. Several units can be combined to form a larger, synchronized system continuing up to 9 OPXs with the current version (90 analog outputs, 90 digital outputs, and 18 analog inputs) and the upcoming version will support many more.

The Quantum Orchestration Platform (QOP) normally replaces most AWGs and acquisition systems in the lab, but can still interface with other instruments via the use of external triggers that can be sent and received to and from other equipment in the lab. In the future, it will also be possible to interface via USB and other interfaces.

Yes. It is possible to use external triggers that can be sent and received to and from other devices in the lab. You may use 10MHz, 100MHz, and 1000MHz to clock the OPX.